Dynamic reconstruction of a calibration state of an absorption spectrometer

ABSTRACT

A reference harmonic absorption curve of a laser absorption spectrometer can have a reference curve shape derived from a reference signal generated by the detector in response to light passing from the laser light source through a reference gas or gas mixture. The reference gas or gas mixture can include one or more of a target analyte and a background gas expected to be present during analysis of the target analyte. A test harmonic absorption curve having a test curve shape is compared with the reference harmonic absorption curve to detect a difference between the test curve shape and the reference curve shape. Operating and/or analytical parameters of the laser absorption spectrometer are adjusted to correct the test curve shape to reduce the difference between the test curve shape and the reference curve shape.

RELATED SUBJECT MATTER

This is a continuation-in-part of U.S. application Ser. No. 13/235,105filed Sep. 16, 2011 and issued on Apr. 29, 2014 as U.S. Pat. No.8,711,357 entitled “Dynamic Reconstruction of a Calibration State of anAbsorption Spectrometer,” which claims priority under 35 U.S.C. §119(e)to U.S. provisional application No. 61/405,589 filed on Oct. 21, 2010and entitled “Dynamic Reconstruction of a Calibration State of anAbsorption Spectrometer.” The current application is also related toco-owned U.S. Pat. No. 7,819,946 entitled “Reactive Gas Detection inComplex Backgrounds,” co-pending and co-owned U.S. patent applicationSer. No. 13/026,921 filed on Feb. 14, 2011 and issued on Jan. 22, 2013as U.S. Pat. No. 8,357,417 entitled “Spectrometer with Validation Cell,”and co-pending and co-owned U.S. patent application Ser. No. 13/027,000filed on Feb. 14, 2011 and issued on Feb. 2, 2015 as U.S. Pat. No.8,953,165 entitled “Validation and Correction of SpectrometerPerformance Using a Validation Cell.” The entirety of the disclosure ofeach application or patent listed in this paragraph is incorporated byreference herein.

TECHNICAL FIELD

The subject matter described herein generally relates to laserspectroscopy and the calibration of absorption spectrometers.

BACKGROUND

Frequency stabilization of a tunable laser light source can be criticalfor quantitative trace gas absorption spectroscopy. Depending on theoperational wavelength, a tunable laser source such as a diode laserscan typically exhibit a wavelength drift on the order of a fewpicometers (on the order of gigahertz) per day to fractions ofpicometers per day. A typical trace gas absorption linewidth can in someinstances be on the order of a fraction of a nanometer to microns. Thus,drift of the laser light source can, over time, introduce criticalerrors in identification and quantification of trace gas analytes,particularly in gas having one or more background compounds whoseabsorption spectra might interfere with absorption features of a targetanalyte.

SUMMARY

In one aspect of the currently described subject matter, a methodincludes retrieving, for example from a computer-readable storage mediumor device, at least one reference harmonic absorption curve of a laserabsorption spectrometer that includes a tunable laser light source and adetector. Each reference harmonic absorption curve has a reference curveshape and includes a first, second, or higher order harmonic signal of areference signal generated by the detector in response to light passingfrom the laser light source through a reference gas or gas mixture. Thereference gas or gas mixture includes one or more of a target analyteand a background gas expected to be present during analysis of thetarget analyte. The reference harmonic absorption curve is determinedfor the laser absorption spectrometer in a known or calibrated state,reflecting the laser scanning behavior in the spectroscopic wavelengthspace and the resulting, calibrated, quantification of the absorptionsignal. A test harmonic absorption curve having a test curve shape iscompared with the at least one reference harmonic absorption curve todetect a difference between the test curve shape and the reference curveshape that exceeds a predefined allowed deviation and thereforeindicates a change in an output of the laser light source and thedetection circuit relative to the calibrated state. One or moreoperating and analytical parameters of the laser absorption spectrometerand the detector circuit are adjusted to correct the test curve shape toreduce the difference between the test curve shape and the referencecurve shape.

In interrelated aspects of the current subject matter, an apparatus caninclude a tangibly embodied machine-readable medium operable to orotherwise storing instructions that cause one or more machines (e.g.,computers, programmable processors, etc.) to perform operations asdescribed herein. Similarly, computer systems are also described thatmay include at least one processor and a memory coupled to the at leastone processor. The memory may include one or more programs that causethe at least one processor to perform one or more of the operationsdescribed herein. A spectrometer can include a machine readable medium,at least one processor, a light source, and a detector.

In optional variations, one or more additional features, including butnot necessarily limited to those described in this and the followingparagraphs of this section of the application, can also be included. Afield validation metric of the laser absorption spectrometer thatincludes at least one of the difference between the test curve shape andthe reference curve shape, an identification of the one or moreoperating and analytical parameters that were adjusted, and a value bywhich the one or more operating and analytical parameters were adjustedcan be promoted. The promoting can include, but is not limited to, oneor more of displaying on a display device of a computing system orportable device, sending an electronic alert message over a network to adevice or user, generating a alert (i.e. visual, auditory, tactile,etc.), generating a telephonic or facsimile transmission, storing analert message and/or associated data to a computer-readable storagemedium, and the like.

The one or more operating and analytical parameters of the laserabsorption spectrometer can include at least one of laser light sourceparameters, detector parameters, and signal conversion parameters usedin generating the test harmonic absorption curve from a signal producedby the detector. The laser light source parameters can include at leastone of a temperature, an operating current, a modulation current, amodulation current frequency, a modulation current amplitude profile, amodulation current frequency profile, a ramp current, a ramp currentfrequency, a ramp current frequency profile, a ramp current amplitudeprofile, an optical beam profile and an optical power. The detectioncircuit parameters can include at least one of a gain and a phasesetting and measurement timing of the detection circuit with respect tothe laser frequency modulation. The signal conversion parameters caninclude at least one of a gain and a phase setting and a timing settingof the demodulating device.

The output can include a light intensity as a function of wavelengthover a wavelength scan range. The laser light source can include atleast one of a tunable diode laser, a tunable semiconductor laser, aquantum cascade laser, an intra-band cascade laser (ICL) a verticalcavity surface emitting laser (VCSEL), a horizontal cavity surfaceemitting laser (HCSEL), a distributed feedback laser, a light emittingdiode (LED), a super-luminescent diode, an amplified spontaneousemission (ASE) source, a gas discharge laser, a liquid laser, a solidstate laser, a fiber laser, a color center laser, an incandescent lamp,a discharge lamp, a thermal emitter, a device capable of generatingfrequency tunable light through nonlinear optical interactions (e.g. viaa Raman method, optical parametric oscillation, etc.), and the like. Thedetector can include for example, one or more of an indium galliumarsenide (InGaAs) detector, an indium arsenide (InAs) detector, anindium phosphide (InP) detector, a silicon (Si) detector, a silicongermanium (SiGe) detector, a germanium (Ge) detector, a mercury cadmiumtelluride detector (HgCdTe or MCT), a lead sulfide (PbS) detector, alead selenide (PbSe) detector, a thermopile detector, a multi-elementarray detector, a single element detector, a photo-multiplier, and thelike. The laser absorption spectrometer can further include a signaldetection circuit that allows adjustment of a signal phase of the laserlight source with respect to a modulation current phase. The laserabsorption spectrometer can further include a signal detection circuitthat allows adjustment of frequency filters. The laser absorptionspectrometer can further include a signal detection circuit that allowsadjustment of DC and AC gain. The laser absorption spectrometer mayfurther include a laser frequency stabilization circuit based upon asuitable molecular absorption line. The laser absorption spectrometercan optionally further include a laser frequency stabilization circuitbased upon a suitable optical system generating optical wavelengthtransmission markers with well defined wavelength spacing.

The comparing can further include applying a curve fitting algorithm toquantify the difference between the test curve shape and the referencecurve shape. The comparing can further include applying at least one ofsubtracting, dividing, cross correlation, curve fitting, andmultivariable regression for one or more parts or the entire of the testcurve and the reference curve, and computing one or more of thedifference, the ratio, the mean square error (MSE), the coefficient ofdetermination (R2), the cross correlation function/integral and theregression coefficients in the light intensity (i.e., the y-axis) and/orthe wavelength (i.e. the x-axis) domain to quantify the differencebetween the test curve shape and the reference curve shape.

The reference curve can include at least one of a calibration referencecurve stored during calibration of the laser absorption spectrometer anda curve constructed using one or more stored calibration referencecurves selected according to a composition of the background gas and/orthe concentration of the target analyte. The method can further includeobtaining the test harmonic absorption curve, which can include passinglight comprising a scanned wavelength range and an imposed modulationfrequency from the light source through a volume of gas, and convertinga signal from the detector to the test harmonic curve. The convertingcan include demodulating the signal at the first, the second, or thehigher order harmonic frequency of the imposed modulation frequency. Theconverting can make use of more than one harmonic order of the signal.

The volume of gas can include one of a sample cell filled with a testgas comprising a known or unknown concentration of the target analyte,the sample cell filled with the background gas, a reference gas volumedisposed in a path of the light and containing the test gas with theknown or unknown concentration of the target analyte, and the referencegas volume disposed in the path of the light and containing only thebackground gas or gas mixture. The sample cell can include a simple passthrough with the laser beam reaching the optical detector withoutoptical reflection of the laser beam. The sample cell can include amultiple-pass configuration in which the light is reflected between oneor more optically reflective mirrors while the light remains inside thesample cell. The sample cell can include a multiple pass configurationrouting the beam by refractive optical means. The sample cell caninclude at least one of a Herriot Cell, an off axis optical resonatorcell and a super high finesse optical cavity.

The method can further include checking fidelity of the laser absorptionspectrometer by one or more of analyzing a premixed calibration samplefrom a premixed container, a prepared calibration sample generated usinga permeation device, a non absorbing zero gas, and a non absorbing zerogas contained in a reference volume.

The details of one or more variations of the subject matter describedherein are set forth in the accompanying drawings and the descriptionbelow. Other features and advantages of the subject matter describedherein will be apparent from the description and drawings, and from theclaims.

DESCRIPTION OF DRAWINGS

The accompanying drawings, which are incorporated in and constitute apart of this specification, show certain aspects of the subject matterdisclosed herein and, together with the description, help explain someof the principles associated with the disclosed implementations. In thedrawings,

FIG. 1 illustrates a process flow diagram illustrating aspects of amethod consistent with implementations of the current subject matter;

FIG. 2 illustrates two spectral absorption charts showing an example ofadjusting a middle operating current of a laser light source to shift atest curve to align with a stored reference curve; and

FIG. 3 is two spectral absorption charts showing an example of adjustingone or more operating parameters of a laser light source and/or signalconverting parameters to correct a test curve shape to reduce thedifference between the test curve shape and a reference curve shape.

When practical, similar reference numbers denote similar structures,features, or elements.

DETAILED DESCRIPTION

To address the above-noted and potentially other issues with currentlyavailable solutions, one or more implementations of the current subjectmatter provide methods, systems, articles of manufacture, and the likethat can, among other possible advantages, provide an automated,algorithmic approach that frequency stabilizes a tunable laser lightsource of a laser absorption spectrometer to improve the robustness ofquantitative trace gas concentration measurements by compensating and/orcorrecting for short term ambient changes in analytical conditions aswell as long term drift and aging effects that may adversely affectperformance of the laser absorption spectrometer.

Real time laser frequency stabilization can be achieved in someimplementations by comparing actual absorption spectra collected at thetime of calibration of an instrument with absorption spectra collectedin the field for gas samples without need for a molecular reference celland a separate laser frequency stabilization circuit. Aside fromincreased cost and complexity, a separate laser frequency stabilizationcircuit can also interfere with the actual measurement. The currentsubject matter can reduce cost and complexity while also improvingoperating robustness and measurement fidelity and reproducibilitycompared to previously available spectroscopy approaches based onfrequency stabilization onto a molecular line which is not part of theactual measurement. Using an approach as described herein, informationabout the performance of a laser spectrometer relative to a previousknown or calibrated state can be obtained across the breadth of ascanned wavelength range of a tunable or scannable laser light source.Such an approach can provide substantial improvement relative totechniques that focus only on peak location rather than an entireabsorption curve shape over a broader range of wavelengths.

FIG. 1 shows a process flow chart 100 illustrating features consistentwith an implementation of the current subject matter. At 102, one ormore reference harmonic absorption curves that can be obtained throughanalysis of one or more reference gas mixtures by a laser absorptionspectrometer is/are retrieved, for example from local or networked datastorage. The one or more reference harmonic absorption curves that canhave been previously obtained through analysis of one or more referencegas mixtures by a laser absorption spectrometer, for example at factorycalibration or at another time when the laser absorption spectrometer isin a well-calibrated state, and stored for later retrieval. At 104, atest harmonic absorption curve is compared with the at least one of theone or more reference harmonic absorption curves to detect a differencebetween the respective curve shapes that exceeds a predefined alloweddeviation. At 106, the operating and/or analytical parameters of thelaser absorption spectrometer are adjusted to correct the test harmonicabsorption curve to reduce the detected difference between the testharmonic absorption curve shape and the reference harmonic absorptioncurve shape. In other words, after adjusting of the one or moreoperating and/or analytical parameters of the laser absorptionspectrometer, a subsequent test harmonic absorption curve more closelyresembles the reference harmonic absorption curve. Optionally, at 110, afield validation metric of the laser absorption spectrometer can bepromoted. The field validation metric can include at least one of thedifference between the test curve shape and the reference curve shape,an identification of the one or more operating and analytical parametersthat were adjusted, and a value by which the one or more operating andanalytical parameters were adjusted.

The adjusting of the one or more operating and/or analytical parametersof the laser absorption spectrometer to reduce the detected differencebetween the test harmonic absorption curve shape and the referenceharmonic absorption curve shape can be performed by a variety ofapproaches. In one implementation, an iterative approach can be used. Inone non-limiting implementation, one of several potential operatingand/or analytical parameters of the laser absorption spectrometer can beadjusted and a new test harmonic absorption curve generated by the laserabsorption spectrometer. Adjustments to the selected parameter cancontinue with successive generation of new test harmonic absorptioncurves until a setting of maximum improvement in the difference betweena test harmonic absorption curve and the reference harmonic absorptioncurve is obtained. Then another parameter can be iteratively adjusted ina similar manner until each parameter has been so adjusted. Anyalgorithm usable for iteratively converging to a multi-variate solutioncan be used.

The test curve can be collected using a reference gas with knownconcentration of a target analyte, or with a sample gas having a knownor unknown concentration of the analyte or even not containing theanalyte (i.e., only the background gas or mixture). If the test curve iscollected with a unknown concentration of the target analyte, areference curve can be constructed using one or more stored referencecurves according to a previously measured target analyte concentration(i.e. the target analyte concentration obtained for a measurementimmediately or otherwise proceeding the current measurement) and thencompare the test curve with the constructed reference curve.Alternatively, only part of the test curve that is not affected by theconcentration of the analyte can be compared. For example, the part ofthe curve that arises only due to absorption of the background gases.

The exact shape of the test curve, and the concentration calculation ofthe one or more target analytes for which the laser absorptionspectrometer is configured to analyze can depend critically upon thelaser frequency behavior. The laser frequency behavior can be affectedby one or more operating and environmental parameters that can include,but are not limited to the center frequency, the ramp current, themodulation current, and other parameters of the laser light source aswell as one or more parameters of the sample cell, detector,demodulator, and the like. The center frequency of the laser lightsource can be affected by at least the operating temperature and theoperating current of the laser light source. The particular frequencychanges caused by changes in drive and/or modulation current,temperature, and the like can be quite specific to each individual laserlight source.

A curve correlation algorithm according to implementations of thecurrent subject matter can generate an error signal whenever the laserfrequency changes, (i.e. if the same reference gas that was used torecord the original reference trace is periodically analyzed). Thereference harmonic absorption curve can be stored once, when theanalyzer receives its original calibration in the factory. Alternativelyor in addition, the reference harmonic absorption curve can be updatedperiodically using a differential spectroscopy approach, for example asdescribed in co-owned U.S. Pat. No. 7,819,946 to adjust for streamchanges, while maintaining a basic reference from the originalcalibration.

Upon receiving an error signal, an optimization algorithm can engage toadjust or otherwise reset one or more operating and analyticalparameters of the laser absorption spectrometer, which can include butare not limited to laser temperature, operating current, modulationcurrent, ramp current, and other signal detection and conversionparameters, to automatically reconstruct the exact harmonic absorptioncurve shape as was originally stored during factory calibration

FIG. 2 and FIG. 3 show two examples of dynamic corrections to acalibration state of a spectrometer using sample data. The referencecurve shown in the top and bottom panels of FIG. 2 is obtained with atunable diode laser spectrometer for a reference gas mixture containingapproximately 25% ethane and 75% ethylene. The test curve shown on thetop panel of FIG. 2 is obtained using the same spectrometer after sometime had passed for a test gas mixture containing 1 ppm acetylene in abackground of approximately 25% ethane and 75% ethylene. Acetylene has aspectral absorption feature in the range of about 300 to 400 on thewavelength axis of the charts in FIG. 2. In an example in which driftand/or other factors affect the spectrometer performance over time, thetest curve can be shifted (for example to the left as shown in FIG. 2)compared with the reference curve. Absent a correction to the testcurve, the measured concentration of acetylene from the spectrometerwould be −0.29 ppm instead of the correct value of 1 ppm.

According to an approach consistent with implementations of the currentsubject matter, the amount of the test curve drift can be identified bycomparing the test and reference curves in a portion of the spectrumoutside of the area where the acetylene absorption feature occurs (i.e.the region between about 20-260 on the wavelength axis). The lasermiddle operating current can be adjusted to shift the test curve back toalign up with the reference curve as shown in the bottom panel of FIG.2. After the adjustment, the measured concentration of acetylene fromthe spectrometer is 1 ppm.

The reference curve in the top and bottom panels of FIG. 3 is alsoobtained with a tunable diode laser spectrometer for a reference gasmixture containing approximately 25% ethane and 75% ethylene. The testcurve on the top panel of FIG. 3 was obtained for a test gas mixturecontaining 1 ppm acetylene in a background of approximately 25% ethaneand 75% ethylene. As shown in the top panel of FIG. 3, the test curveshape is distorted relative to the shape of the reference curve due todrift or other factors affecting performance of the laser absorptionspectrometer over time. If the test curve is not corrected, the measuredconcentration of acetylene in the test gas mixture determined by thespectrometer can be, for example, 1.81 ppm instead of the trueconcentration of 1 ppm.

According to an approach consistent with implementations of the currentsubject matter, the amount of test curve distortion can be identifiedand/or corrected for by comparing one or more sections of the test curveand reference curve in one or more portions of the spectrum outside ofthe area where the acetylene absorption feature occurs (i.e. the regionsbetween about 20-260 and 400-500 on the wavelength axis). The laseroperating parameters and signal converting parameters can be adjusted tocorrect the test curve shape to more closely resemble the referencecurve shape. After the adjustment, the measured concentration ofacetylene from the spectrometer turns to 1 ppm.

The approaches illustrated in FIG. 2 and FIG. 3 use a reference harmonicspectrum collected for a sample having a background compositionconsistent with that expected to be present under analytical conditionsduring which the target analyte (acetylene) is to be quantified. In analternative or additional implementation, the reference harmonic spectracan be selected to contain one or more background absorption peaks thatdo not change with background compositions. In an alternative oradditional implementation, the reference harmonic spectrum can beconstructed from reference absorption spectra of individual backgroundspecies.

As described and illustrated, implementations of the current subjectmatter can consider substantially more information regarding the exactshape of a reference harmonic absorption curve than is typically used inpeak locking. Previously available laser control loops are generallylimited to only stabilizing or tracking the laser frequency and/or peakposition (i.e. location of the peak of a spectral feature in thedigitized scan range of the measurement).

The approach described herein can be applicable to any laser absorptionspectrometer that includes a tunable laser source, including but notlimited to direct absorption spectrometers, harmonic absorptionspectrometers, differential absorption spectrometers, etc. For a directabsorption spectrometer, the measurement of target analyteconcentrations can be performed without using a harmonic conversion ordemodulation of the signal obtained from the detector. However, periodicor continuous recalibration of the laser light source, detector, etc.can be performed using a calibration circuit, etc. that makes use of aharmonic signal obtained from the detector signal.

In another implementation, the calibration state of a harmonicabsorption spectrometer can be validated using different operatingparameters, including but not limited to the modulation frequency, rampfrequency, etc., than are used in identifying and/or quantifying atarget analyte. Use of larger modulation frequencies can increase thesignal to noise ratio of an absorption feature of a target analyte byrelatively reducing the impact of absorption by the backgroundcomposition of a gas mixture. However, as the current subject matter canmake use of information obtained from all absorption features that occuracross a laser scan range in verifying agreement between a test harmonicabsorption curve and a reference harmonic absorption curve, it can beadvantageous to collect both the test and reference harmonic absorptioncurves under conditions that lead to a more complicated spectrum so thatadditional features are available to be matched between the test andreference harmonic absorption curves.

Aspects of the subject matter described herein can be embodied insystems, apparatus, methods, and/or articles depending on the desiredconfiguration. In particular, various implementations of the subjectmatter described herein can be realized in analog or digital electroniccircuitry, integrated circuitry, specially designed application specificintegrated circuits (ASICs), computer hardware, firmware, software,and/or combinations thereof. These various implementations can includeimplementation in one or more computer programs that are executableand/or interpretable on a programmable system including at least oneprogrammable processor, which can be special or general purpose, coupledto receive data and instructions from, and to transmit data andinstructions to, a storage system, at least one input device, and atleast one output device.

These computer programs, which can also be referred to as programs,software, software applications, applications, components, or code,include machine instructions for a programmable processor, and can beimplemented in a high-level procedural and/or object-orientedprogramming language, and/or in assembly/machine language. As usedherein, the term “machine-readable medium” refers to any computerprogram product, apparatus and/or device, such as for example magneticdiscs, optical disks, memory, and Programmable Logic Devices (PLDs),used to provide machine instructions and/or data to a programmableprocessor, including a machine-readable medium that receives machineinstructions as a machine-readable signal. The term “machine-readablesignal” refers to any signal used to provide machine instructions and/ordata to a programmable processor. The machine-readable medium can storesuch machine instructions non-transitorily, such as for example as woulda non-transient solid state memory or a magnetic hard drive or anyequivalent storage medium. The machine-readable medium can alternativelyor additionally store such machine instructions in a transient manner,such as for example as would a processor cache or other random accessmemory associated with one or more physical processor cores.

To provide for interaction with a user, the subject matter describedherein can be implemented on a computer having a display device, such asfor example a cathode ray tube (CRT) or a liquid crystal display (LCD)monitor for displaying information to the user and a keyboard and apointing device, such as for example a mouse or a trackball, by whichthe user may provide input to the computer. Other kinds of devices canbe used to provide for interaction with a user as well. For example,feedback provided to the user can be any form of sensory feedback, suchas for example visual feedback, auditory feedback, or tactile feedback;and input from the user may be received in any form, including, but notlimited to, acoustic, speech, or tactile input. Other possible inputdevices include, but are not limited to, touch screens or othertouch-sensitive devices such as single or multi-point resistive orcapacitive trackpads, voice recognition hardware and software, opticalscanners, optical pointers, digital image capture devices and associatedinterpretation software, and the like.

The subject matter described herein can be implemented in a computingsystem that includes a back-end component, such as for example one ormore data servers, or that includes a middleware component, such as forexample one or more application servers, or that includes a front-endcomponent, such as for example one or more client computers having agraphical user interface or a Web browser through which a user caninteract with an implementation of the subject matter described herein,or any combination of such back-end, middleware, or front-endcomponents. A client and server are generally, but not exclusively,remote from each other and typically interact through a communicationnetwork, although the components of the system can be interconnected byany form or medium of digital data communication. Examples ofcommunication networks include, but are not limited to, a local areanetwork (“LAN”), a wide area network (“WAN”), and the Internet. Therelationship of client and server arises by virtue of computer programsrunning on the respective computers and having a client-serverrelationship to each other.

The implementations set forth in the foregoing description do notrepresent all implementations consistent with the subject matterdescribed herein. Instead, they are merely some examples consistent withaspects related to the described subject matter. Although a fewvariations have been described in detail herein, other modifications oradditions are possible. In particular, further features and/orvariations can be provided in addition to those set forth herein. Forexample, the implementations described above can be directed to variouscombinations and sub-combinations of the disclosed features and/orcombinations and sub-combinations of one or more features further tothose disclosed herein. In addition, the logic flows depicted in theaccompanying figures and/or described herein do not necessarily requirethe particular order shown, or sequential order, to achieve desirableresults. The scope of the following claims may include otherimplementations or embodiments.

What is claimed:
 1. A method for implementation by one or more dataprocessors comprising: retrieving, by at least one data processor, areference harmonic absorption curve of a laser absorption spectrometer,the laser absorption spectrometer comprising a tunable or scannablelaser light source and a detector, the reference harmonic absorptioncurve having a reference curve shape and comprising a first, second, orhigher order harmonic signal of a reference signal generated by thedetector in response to light passing from the laser light sourcethrough a reference gas or gas mixture, the reference gas or gas mixturecomprising one or more of a target analyte and a background gas expectedto be present during analysis of the target analyte, the referenceharmonic absorption curve having been determined for the laserabsorption spectrometer in a known or calibrated state; comparing, by atleast one data processor, at least one portion of a test harmonicabsorption curve having a test curve shape with at least one portion ofthe reference harmonic absorption curve to detect a difference betweenthe test curve shape and the reference curve shape that exceeds apredefined allowed deviation and therefore indicates a change in anoutput of the laser light source relative to the known or calibratedstate, wherein one or more portions of the test harmonic absorptioncurve is compared with one or more portions of the reference harmonicabsorption curve arising due to absorption of the background gases andnot by absorption of the target analyte; and causing, by at least onedata processor, one or more operating and analytical parameters of thelaser absorption spectrometer to be adjusted based on the comparing. 2.A method as in claim 1, further comprising promoting, by at least onedata processor, a field validation metric of the laser absorptionspectrometer, the field validation metric comprising at least one of thedifference between the test curve shape and the reference curve shape,an identification of the one or more operating and analytical parametersthat were adjusted, and a value by which the one or more operating andanalytical parameters were adjusted.
 3. A method as in claim 1, whereinthe one or more operating and analytical parameters of the laserabsorption spectrometer comprise at least one of laser light sourceparameters, detector parameters, and signal conversion parameters usedin generating the test harmonic absorption curve from a signal producedby the detector.
 4. A method as in claim 3, wherein the laser lightsource parameters comprise at least one of a temperature, an operatingcurrent, a modulation current, a ramp current, and a phase of the laserlight source; the detector parameters comprise at least one of a gainand a phase setting of a detector circuit; and the signal conversionparameters comprise at least one of a gain and a phase setting of ademodulating device.
 5. A method as in claim 1, wherein the outputcomprises a light intensity as a function of wavelength over awavelength scan range.
 6. A method as in claim 1, wherein the lightsource comprises at least one of a tunable diode laser, a tunablesemiconductor laser, a quantum cascade laser, an intra-band cascadelaser (ICL) a vertical cavity surface emitting laser (VCSEL), ahorizontal cavity surface emitting laser (HCSEL), a distributed feedbacklaser, a light emitting diode (LED), a super-luminescent diode, anamplified spontaneous emission (ASE) source, a gas discharge laser, aliquid laser, a solid state laser, a fiber laser, a color center laser,an incandescent lamp, a discharge lamp, a thermal emitter, and a devicecapable of generating frequency tunable light through nonlinear opticalinteractions; and the detector comprises at least one of an indiumgallium arsenide (InGaAs) detector, an indium arsenide (InAs) detector,an indium phosphide (InP) detector, a silicon (Si) detector, a silicongermanium (SiGe) detector, a germanium (Ge) detector, a mercury cadmiumtelluride detector (HgCdTe or MCT), a lead sulfide (PbS) detector, alead selenide (PbSe) detector, a thermopile detector, a multi-elementarray detector, a single element detector, and a photo-multiplier.
 7. Amethod as in claim 1, wherein the comparing further comprises applying acurve fitting algorithm to quantify the difference between the testcurve shape and the reference curve shape.
 8. A method as in claim 1,wherein the comparing further comprises applying at least one ofsubtracting, dividing, cross correlation, curve fitting, andmultivariable regression for one or more parts or the entirety of thetest curve and the reference curve, and computing one or more of thedifference, the ratio, the mean square error (MSE), the coefficient ofdetermination (R²), the cross correlation function/integral and theregression coefficients in the light intensity (i.e., the y-axis) and/orthe wavelength (i.e. the x-axis) domain to quantify the differencebetween the test curve shape and the reference curve shape.
 9. A methodas in claim 8, wherein the reference curve comprises at least one of acalibration reference curve stored during calibration of the laserabsorption spectrometer and a curve constructed using one or more storedcalibration reference curves selected according to a composition of thebackground gas and/or the concentration of the target analyte.
 10. Amethod as in claim 1, further comprising obtaining the test harmonicabsorption curve, the obtaining comprising: passing light from the lightsource through a volume of gas, the light comprising a scannedwavelength range and an imposed modulation frequency; and converting asignal from the detector to the test harmonic curve, the convertingcomprising demodulating the signal at the first, the second or thehigher order harmonic frequency of the imposed modulation frequency. 11.A method as in claim 1 wherein the volume of gas comprises one of asample cell filled with a test gas comprising a known or unknownconcentration of the target analyte, the sample cell filled with thebackground gas, a reference gas volume disposed in a path of the lightand containing the test gas with the known or unknown concentration ofthe target analyte, and the reference gas volume disposed in the path ofthe light and containing only the background gas or gas mixture.
 12. Amethod as in claim 11, wherein the sample cell comprises at least one ofa multiple-pass configuration in which the light is reflected betweenone or more optically reflective mirrors while the light remains insidethe sample cell; a multiple-pass configuration in which the light isrefracted by one or more optical elements while the light remains insidethe sample cell; a Herriot Cell; an off-axis optical resonator; a Whitecell; an optical cavity; a hollow core light guide; and a single passconfiguration in which the light is not being reflected while the lightremains inside the sample cell.
 13. A method as in claim 1, furthercomprising checking fidelity of the laser absorption spectrometer by oneor more of analyzing a premixed calibration sample from a premixedcontainer, a prepared calibration sample generated using a permeationdevice, a non-absorbing zero gas, and a non-absorbing zero gas containedin a reference volume.
 14. A method as in claim 1, wherein the laserabsorption spectrometer further comprises a signal detection circuitthat allows at least one of adjustment of a signal phase with respect toa modulation current phase of the laser light source, adjustment offrequency filters, and adjustment of DC and AC gain.
 15. An apparatuscomprising: a non-transitory machine-readable storage medium storinginstructions that, when executed by at least one processor, cause the atleast one processor to perform operations comprising: retrieving areference harmonic absorption curve of a laser absorption spectrometer,the laser absorption spectrometer comprising a tunable or scannablelaser light source and a detector, the reference harmonic absorptioncurve having a reference curve shape and comprising a first, second, orhigher order harmonic signal of a reference signal generated by thedetector in response to light passing from the laser light sourcethrough a reference gas or gas mixture, the reference gas or gas mixturecomprising one or more of a target analyte and a background gas expectedto be present during analysis of the target analyte; the referenceharmonic absorption curve having been determined for the laserabsorption spectrometer in a known or calibrated state; comparing atleast one portion of a test harmonic absorption curve having a testcurve shape with at least one portion of the reference harmonicabsorption curve to detect a difference between the test curve shape andthe reference curve shape that exceeds a predefined allowed deviationand therefore indicates a change in an output of the laser light sourcerelative to the known or calibrated state, wherein one or more portionsof the test harmonic absorption curve is compared with one or moreportions of the reference harmonic absorption curve arising due toabsorption of the background gases and not by absorption of the targetanalyte; and causing one or more operating and analytical parameters ofthe laser absorption spectrometer to be adjusted based on the comparing.16. An apparatus as in claim 15, further comprising the at least oneprocessor.
 17. An apparatus as in claim 15, further comprising the laserabsorption spectrometer.
 18. An apparatus as in claim 17, wherein thelight source comprises at least one of a tunable diode laser, a tunablesemiconductor laser, a quantum cascade laser, an intra-band cascadelaser (ICL), a vertical cavity surface emitting laser (VCSEL), ahorizontal cavity surface emitting laser (HCSEL), a distributed feedbacklaser, a light emitting diode (LED), a super-luminescent diode, anamplified spontaneous emission (ASE) source, a gas discharge laser, aliquid laser, a solid state laser, a fiber laser, a color center laser,an incandescent lamp, a discharge lamp, a thermal emitter, and a devicecapable of generating frequency tunable light through nonlinear opticalinteractions; and the detector comprises at least one of an indiumgallium arsenide (InGaAs) detector, an indium arsenide (InAs) detector,an indium phosphide (InP) detector, a silicon (Si) detector, a silicongermanium (SiGe) detector, a germanium (Ge) detector, a mercury cadmiumtelluride detector (HgCdTe or MCT), a lead sulfide (PbS) detector, alead selenide (PbSe) detector, a thermopile detector, a multi-elementarray detector, a single element detector, and a photo-multiplier. 19.An apparatus as in claim 17, wherein the volume of gas comprises one ofa sample cell filled with a test gas comprising a known or unknownconcentration of the target analyte, the sample cell filled with thebackground gas, a reference gas volume disposed in a path of the lightand containing the test gas with the known or unknown concentration ofthe target analyte, and the reference gas volume disposed in the path ofthe light and containing only the background gas or gas mixture.
 20. Anapparatus as in claim 19, wherein the sample cell comprises at least oneof a multiple-pass configuration in which the light is reflected betweenone or more optically reflective mirrors while the light remains insidethe sample cell; a multiple-pass configuration in which the light isrefracted by one or more optical elements while the light remains insidethe sample cell; a Herriot Cell; an off-axis optical resonator; a Whitecell; an optical cavity; a hollow core light guide; and a single passconfiguration in which the light is not being reflected while the lightremains inside the sample cell.
 21. An apparatus as in claim 17, whereinthe laser absorption spectrometer further comprises a signal detectioncircuit that allows at least one of adjustment of a signal phase withrespect to a modulation current phase of the laser light source,adjustment of frequency filters, and adjustment of DC and AC gain. 22.An apparatus as in claim 15, wherein the one or more operating andanalytical parameters of the laser absorption spectrometer comprise atleast one of laser light source parameters, detector parameters, andsignal conversion parameters used in generating the test harmonicabsorption curve from a signal produced by the detector.
 23. Anapparatus as in claim 22, wherein the laser light source parameterscomprise at least one of a temperature, an operating current, amodulation current, a ramp current, and a phase of the laser lightsource; the detector parameters comprise at least one of a gain and aphase setting of a detector circuit; and the signal conversionparameters comprise at least one of a gain and a phase setting of ademodulating device.
 24. An apparatus as in claim 15, wherein the outputcomprises a light intensity as a function of wavelength over awavelength scan range.
 25. An apparatus comprising: means for generatingor receiving a reference harmonic absorption curve of a laser absorptionspectrometer, the laser absorption spectrometer comprising a tunable orscannable laser light source and a detector, the reference harmonicabsorption curve having a reference curve shape and comprising a first,second, or higher order harmonic signal of a reference signal generatedby the detector in response to light passing from the laser light sourcethrough a reference gas or gas mixture, the reference gas or gas mixturecomprising one or more of a target analyte and a background gas expectedto be present during analysis of the target analyte, the referenceharmonic absorption curve having been determined for the laserabsorption spectrometer in a known or calibrated state; means forcomparing at least one portion of a test harmonic absorption curvehaving a test curve shape with at least one portion of the referenceharmonic absorption curve to detect a difference between the test curveshape and the reference curve shape that exceeds a predefined alloweddeviation and therefore indicates a change in an output of the laserlight source relative to the known or calibrated state, wherein one ormore portions of the test harmonic absorption curve is compared with oneor more portions of the reference harmonic absorption curve arising dueto absorption of the background gases and not by absorption of thetarget analyte; and means for causing one or more operating andanalytical parameters of the laser absorption spectrometer to beadjusted based on the comparing.